Field Transformations: loop moving along wire

AI Thread Summary
When a loop moves with velocity v along a stationary charged wire, the electric field (E) at a point on the loop is derived from the wire's charge density and includes the cross product of the loop's velocity with the magnetic field (B'), which is zero due to the absence of current. Conversely, when the wire moves with velocity -v and the loop is stationary, the E field at the loop is influenced by the wire's electric field and the cross product of the wire's velocity with the electric field (E'). In this scenario, the B field is adjusted by subtracting the cross product of the wire's velocity and the electric field from the B field of a current-carrying wire. The discussion emphasizes the transformation of electric and magnetic fields based on the relative motion of the loop and the wire. Understanding these field transformations is crucial for solving problems in electromagnetism.
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Homework Statement


A loop moves with velocity v along a charged wire. (The charged wire passes through the center of the loop.)

In a reference frame where the charged wire is stationary and the loop is moving with v, what is the E field and B field at a point on the loop?

In a reference frame where the charged wire is moving with -v and the loop is stationary, what is the E field and B field at a point on the loop?

Homework Equations



E'= E + V x B
B' = B - (1/c^2)V x E

The Attempt at a Solution


When the charged wire is stationary and the loop is moving with v, is the E equal to the E of a point from a charged wire plus the cross product of velocity and the magnetic field B' (the B' in ref frame where wire is moving and a current does exist)?
That is E = \lambda/(2\pi\epsilonr) + V x B' ...where lamda is charge density of the wire, and where B'=\muI/(2\pir)
And is the B simply 0 because there is no current?

p.s. sorry don't know why latex is doing that but there's no superscripts in the equations
 
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Yes, when the charged wire is stationary and the loop is moving with velocity v, the E field at a point on the loop is equal to the E field from a charged wire plus the cross product of velocity and the magnetic field B'. The B field at this point is simply 0 since there is no current.When the charged wire is moving with velocity -v and the loop is stationary, the E field at a point on the loop is equal to the E field from a charged wire plus the cross product of velocity and the electric field E'. The B field at this point is equal to the B field from a current carrying wire minus the cross product of velocity and the electric field E'.
 
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